/ Hiroyuki Sagawa / Professor
/ Hisasi Morikawa / Professor
/ Ken-ichi Funahashi / Associate Professor
/ Katsutaro Shimizu / Associate Professor
/ Kazuto Asai / Assistant Professor
/ Michio Honma / Assistant Professor
/ Shigeru Watanabe / Assistant Professor
/ Toshiro Watanabe / Assistant Professor
/ Hiroshi kihara / Research Associate
The scope of activities of the Center for Mathematical sciences spans all aspects of education and research in the fields of mathematical sciences. Current research directions in the field of mathematics are joined by the common theme ``Geometrical Method in Mathematical Sciences". In the fields of Physics, theoretical research is performed in many-body theories, Nuclear Physics and Quantum Gravity. Together with this, there is a project to develop educational software on quantum physics. The research areas assigned to each co-researcher are as follows:
Refereed Journal Papers
Reaction cross sections and root-mean-square (rms) radii of $A$=17 and $A$=20 isobars are calculated by using a simplified Glauber model and spherical and deformed Hartree-Fock (HF) wave functions. The small separation energy effect is discussed on the reaction cross sections of $A$=17 isobars and possible proton halo in $^{17}$Ne. The calculated rms mass radii of $A$=20 isobars are increased appreciably by the deformation effect and show a similar irregular pattern as a function of the isospin to that of the observed radii.
We study the giant quadrupole resonances in the neutron drip line nucleus, $^{28}_{8}O_{20}$~, using the self-consistent Hartree-Fock calculation plus the random phase approximation with Skyrme interactions. Including simultaneously both the isoscalar and the isovector correlation the RPA response function is calculated in the coordinate space so as to take into account properly the continuum effect. Though in neutron drip line nuclei the distribution of the quadrupole strength is much affected by the presence of the low-energy threshold strength, the isoscalar and the isovector correlation structure as well as the transition densities of the isoscalar giant resonance are in good agreement with those given by the collective model. In contrast, the transition density of the isovector giant resonance shows a clear deviation from that of the liquid-drop polarization mode.
Excitation energies, branching ratios and E2/M1 mixing ratios of the negative-parity states in $^{125,127}$Xe and $^{125,127,129}$Cs have been calculated by using the proton-neutron Interacting Boson Fermion Model (IBFM2). A good agreement with the experiment has been obtained. The sensitivity of the calculated observables to changes in model parameters is discussed and the results are compared with those obtained from the IBFM1. We examine a symmetry of the hamiltonian with respect to the change of sign of the parameters $\chi_{\pi},\chi_{\nu}$ and $\Gamma$. The different behaviours of the odd Xe and Cs isotopes arise from the different position of the proton and neutron Fermi levels. In particular the exchange term of the hamiltonian in $^{125,127,129}$Cs can be neglected.
High-spin states of $^{145}$Sm were studied by using several heavy ion reactions. The excitatione energy and spin-parity of high spin isomers are determined by using the deformed independent particle model.
Using the self-consistent Hartree-Fock calculation plus RPA with Skyrme interactions, the RPA quadrupole strength function is estimated in the coordinate space, including simultaneously both the isoscalar and the isovector correlation. We discuss the result of the isoscalar, the isovector and the electric quadrupole polarization of the Ca-isotopes from the proton drip line towards the neutron drip line. We study also the comparison of the polarizations in the $A\!=\!48$ mirror nuclei, $^{48}_{28}Ni_{20}$ and $^{48}_{20}Ca_{28}$~, and the dependence of the polarizations of $^{28}_{8}O_{20}$ on various Skyrme interactions.
Isoscalar and isovector monopole responses of Ca-isotopes towards drip lines are studied in comparison with those of stable nuclei, $^{40}$Ca, $^{90}$Zr and $^{208}$Pb~, using the self-consistent Hartree-Fock calculation plus the random phase approximation with Skyrme interactions. Including simultaneously both the isoscalar and the isovector correlation the RPA response function is calculated in the coordinate space so as to take properly into account the continuum effect. The distribution of the monopole strength is much affected by the presence of the low-energy threshold strength in both proton and neutron drip line nuclei, while the isoscalar monopole strength is concentrated in one giant peak in the heavy $\beta$-stable nucleus $^{208}$Pb. It is found that in drip line nuclei the transition density and the displacement field of protons are very different from those of neutrons, especially around the nuclear surface. The relation between the compression modulus of the nuclear matter $K_{nm}$ and that of finite nuclei $K_{A}$ is also discussed by using the energy moments estimated in RPA.
We study electric dipole transitions between Gamow-Teller (GT) and spin-dipole (SD) states. SD and GT excitations are calculated within the Hartree-Fock (HF) + Tamm- Dancoff approximation (TDA) for $^{48}$Sc and $^{90}$Nb. The electric dipole transitions are found to be rather selective and strong E1 transitions occur to some specific spin-dipole states. Calculated E1 transition strengths between GT and SD states are compared with the analytic sum rules within 1 particle-1 hole (1p-1h) configuration space and within both 1p-1h and 2p-2h model space. Possible implications for charge-exchange reactions may help to understand the quenching problem of spin excitations.
We study the energy dependence of the cross sections for nucleon removal of $^8B$ projectiles. It is shown that the Glauber model calculations with nucleon-nucleon t-matrix reproduce well the energy dependence of the breakup cross sections of $^8B$. A DWBA model for the breakup cross section is also proposed and results are compared with those of the Glauber model. We show that to obtain an agreement between the DWBA calculations, the Glauber formalism, and the experimental data, it is necessary to modify the energy behavior of the effective interaction. In particular, the breakup potential has a quite different energy dependence than the strong absorption potential.
The isoscalar and the isovector dipole mode of drip line and $\beta$-stable nuclei are investigated, using the self-consistent Hartree-Fock plus the random-phase approximation with Skyrme interactions. Including simultaneously both the isoscalar and the isovector correlation, the RPA response function is estimated in the coordinate space so as to take into account properly the continuum effect. The spurious component is carefully taken away from the calculated strength. In $\beta$-stable nuclei such as ~$^{208}Pb$~ the frequency of the isovector giant dipole resonance (IVGDR) is lower than that of the isoscalar giant dipole resonance (compression mode). In contrast, in lighter drip line nuclei a major part of the isoscalar compression dipole strength lies at an energy much lower than the energy of the IVGDR.
Refereed Proceeding Papers
Academic Activities
Others